rotation
to isolate the source and protect the laser oscillator from reflections in an
optical system. In other words, they basically act as an optical diode allowing
the propagation of light in only one direction.
1030-1080nm High Power Free Space Faraday Isolators -
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General specifications:
Clear Aperture: 4 mm
Rotating Medium: TGG
Operating wavelength: 1030 nm - 1080 nm
Rotation Angle at Specified Wavelength : 45Deg +/- 30
Transmission With Polarizers: > 92%
Isolation : >=30dB
Pulsed Damage Threshold for 10nsec pulse: 5J/cm2
Del Mar Photonics - Kirra Faraday Isolator brochure - Faraday Isolator Models
Del Mar Photonics - Newsletter Fall 2010 - Newsletter Winter 2010
At high powers optical feedback can damage or disrupt the operation of a
laser system. To reduce this feedback, an optical isolator can be inserted into
the system. Faraday optical isolators (based on the Faraday effect) are passive
unidirectional, nonreciprocal devices that utilize the phenomenon of
magneto-optic
rotation
to isolate the source and protect the laser oscillator from reflections in an
optical system. In other words, they basically act as an optical diode allowing
the propagation of light in only one direction.
Faraday isolators (see Figure 1) typically consist of a Faraday rotator, two
polarizers, and a body to house the parts. The Faraday rotator, in turn,
consists of magnetooptically active optical material placed inside a permanent
magnet (Nd-Fe-B).
In the Faraday optical isolator shown in Figure 2, the magneto-optical rod
(located inside the Faraday rotator) is cut from glass (MOS-10) polished to
flatness of 
/10, and has parallelism
better than 10 arc seconds.
It
is anti-reflection coated with residual reflection <0.2% (each side) in the
765-835 nm range. The polarizers are air-spaced Glan prisms made of calcite.
Entrance and exit faces of polarizers are anti-reflection coated with residual
reflection of <0.3% in the range. Polarizer transmittance is >98%. This gives a
total transmittance of better than 85% for the isolator.
Laser light (polarized or unpolarized) enters the input polarizer (P1) and is linearly polarized to 0°. Next, the linearly polarized light enters the Faraday rotator rod (magneto-optical rod). The plane of polarization rotates as the light propagates along the axis of the rod. The Faraday rotator is tuned to rotate the plane of polarization by 45°. (Changing the position of the rod allows tuning over a wavelength range from 765-835 nm.) The light then passes through the output polarizer (P2) whose transmission axis is also at 45°.
Any back reflected light re-enters the isolator through the output polarizer and becomes polarized at 45°. The back reflected light then passes through the Faraday rotator, which produces another 45° of rotation, and is now polarized at 90°, or horizontally, before being stopped by the input polarizer, still at 0°. Thus, the laser is isolated from its own reflections that may occur in the application part of the optical set.
This information was contributed by Sergey Egorov for Del Mar Photonics, located in San Diego, CA.
Del Mar Photonics - Kirra Faraday Isolator brochure - Faraday Isolator Models
Broadband Faraday Isolator for Femtosecond Ti:Sapphire Laser
Del Mar Photonics - Kirra Faraday Isolator brochure - Faraday Isolator Models
Wideband isolator model Kirra 5AFI38B-800C has 100 nm band: extinction ratio at
750/850 nm - 35dB, at 800 nm - 38 dB.
Isolation of the broadband Faraday isolator Kirra 5AFI38B-800C for femtosecond Ti:Sapphire laser as a function of wavelength.
Transmission of the broadband Faraday isolator Kirra 5AFI38B-800C for femtosecond Ti:Sapphire laser as a function of wavelength.
Del Mar Photonics - Kirra Faraday Isolator brochure - Faraday Isolator Models